Lab #7: The Carnot Cycle
Reading
Assignment:
Halliday, Resnick, and Walker, Chapter 21, Sections 1-5
Introduction:
In the early nineteenth century, a French scientist, Sadi Carnot (1796-1832) studied the thermodynamic processes in which mechanical energy was obtained from thermal energy. The ideal gas cyclic engine has taken his name and is now called the Carnot cycle. This cycle involves four reversible processes, ie. 4 steps that are carried out infinitely slowly and which can be considered a series of thermodynamic equilibrium states each of which can be reversed with no change in the magnitudes of the work done or heat absorbed.
A typical Carnot cycle is shown in the figure below:

The cycle consists of the following four steps:
For each of the steps, the work done may be calculated depending upon the particular process involved. For any isothermal process the work done is given by:
(isothermal
process) Eq. (1)
where n is the number of moles of gas present and R, known as the Gas Constant, has a value of 8.31 J/mol-K.
Similarly, the work done during an adiabatic process is given by:
(adiabatic
process) Eq. (2)
The resulting efficiency of going around one complete cycle is defined as:
(efficiency)
Eq. (3)
As always, at each point the ideal gas equation holds and the 1st Law of Thermodynamics is valid for each process, ie:
(Ideal gas law) Eq. (4)
and
(1st Law of Thermodynamics)
Eq. (5)
Goals for this
activity:
· To study the various steps in a Carnot cycle
· To calculate the values for Q, W and DEint for each step in the cycle
· To determine the ideal efficiency for a particular Carnot cycle
Lab #7: The
Carnot Cycle
Name:_______________________________ Section #:________
Name:_______________________________
Name:_______________________________
Discussion
Questions:
Consider a cyclic heat engine that undergoes the following cycle using 2 moles of an ideal monatomic gas:
Step A: an isothermal expansion at 727oC from 1 m3 to 4 m3;
Step B: an adiabatic expansion to 327oC;
Step C: an isothermal compression at 327oC; and
Step D: an adiabatic compression back to the initial conditions.
|
|
W (in J) |
DQ (in J) |
DEint (in J) |
|
Step A |
|
|
|
Step B |
|
|
|
Step C |
|
|
|
Step D |
|
|
|
For the cycle |
|
|
|